JP3455987B2 - Quantum box assembly device and information processing method - Google Patents

Description

Detailed Description of the Invention

[0001]

This invention relates to a quantum box assembly device and a quantum box assembly device.
And information processing methods .

[0002]

2. Description of the Related Art In recent years, in quantum wave electronics, a so-called quantum box structure, ie, a so-called quantum box structure having a cross-sectional dimension about the same as the de Broglie wavelength of an electron, has been attracting attention, and it is confined within this quantum box. There is great interest in the quantum effects exhibited by dimensional electrons.

A quantum box assembly element is a combination of a plurality of such quantum boxes and performs information processing by causing quantum mechanical tunneling of electrons between these quantum boxes to change the electron distribution. Is being considered.

[0004]

As described above, the conventional quantum box assembly device performs information processing by conducting electrons between the quantum boxes. If the spaces can be conducted and can be involved in information processing, the degree of freedom in designing the quantum box assembly device can be increased. However, when electrons and holes are simply conducted, electron-hole recombination occurs during conduction, so that the number of electrons and holes involved in conduction is reduced, which causes a problem in operation.

Therefore, an object of the present invention is to perform information processing by conducting electrons and holes respectively without causing recombination during conduction, and a quantum box assembly element and information having a high degree of freedom in design. It is to provide a processing method .

[0006]

In order to achieve the above object, a quantum box assembly element according to the first invention of the present invention comprises a plurality of first quantum boxes (QD ₁ ) provided in a first plane. so
Second , there is a possibility that electrons can be conducted between them .
A plurality of second quantum boxes (QD ₂ ) provided corresponding to the plurality of first quantum boxes (QD ₁ ) in the plane of
Between which electron and hole conduction is not substantially allowed between
And a plurality of third quantum boxes (QD ₃ ) provided corresponding to the plurality of second quantum boxes (QD ₂ ) in the third plane,
And a one conduction holes between them is allowed, more
On the first quantum box (QD ₁ ) side of the plurality of third quantum boxes (QD ₁ )
Bias voltage is set so that the potential becomes higher than that on the D ₃ ) side.
Second quantum box selected by light irradiation in the applied state
By generating an electron-hole pair in (QD ₂ ), an initial charge is generated.
Bias voltage is input by inputting the child distribution and the initial hole distribution.
Of the second quantum box (Q
Corresponds to paired electrons and holes generated in D ₂ )
The first quantum box (QD ₁ ) and the third quantum box (QD 1
₃ ), the initial electron distribution and initial positive
The hole distributions are respectively defined by a plurality of first quantum boxes (QD ₁ ) and
Transfer to multiple _third quantum boxes (QD ₃ ), and then transfer to multiple
Conducting electrons between the first quantum boxes (QD ₁ ) of
To conduct holes between the plurality of third quantum boxes (QD ₃ ).
Performs information processing by Rukoto, the bias voltage substantially
By removing them in the multiple first quantum boxes (QD ₁ ).
The electrons and holes in the _third quantum boxes (QD ₃ )
Into the _second quantum box (QD ₂ ) of
By electron-hole recombination from the _second quantum box (QD ₂ ).
Output by observing luminescence and obtaining luminescence intensity distribution
It is characterized by doing so.

A quantum box ensemble element according to a second invention of the present invention is the quantum box ensemble element according to the first invention of the present invention, wherein the first quantum box (QD ₁ ) and the second quantum box (QD ₁ ).
D ₂ ) and the third quantum box (QD ₃ ) are characterized by being formed by a type I heterojunction superlattice.

A quantum box ensemble element according to a third invention of the present invention is the quantum box ensemble element according to the first or second invention of the present invention, wherein a plurality of first quantum boxes (QD ₁ ) are provided.
A wavelength that resonates with the electron-hole pair generation energy of the second quantum box (QD ₂ ) in the state where a bias voltage is applied so that the side becomes higher potential than the plurality of third quantum boxes (QD ₃ ) side. Of light is applied to the selected second quantum box (QD ₂ ) to generate electron-hole pairs, thereby inputting the initial electron distribution and the initial hole distribution, and increasing the bias voltage to increase the light The electron and hole pair-generated in the second quantum box (QD ₂ ) selected by the incident are respectively generated by the corresponding first
Quantum box (QD ₁₎ and the third quantum boxes (QD ₃₎ initial electron distribution and initial hole distribution plurality of first quantum box by moving the (QD ₁₎ and a plurality of third quantum By transferring to a box (QD ₃ ) and then conducting electrons between a plurality of first quantum boxes (QD ₁ ) and conducting holes between a plurality of third quantum boxes (QD ₃ ). By performing information processing and substantially eliminating the bias voltage, the electrons in the plurality of _first quantum boxes (QD ₁ ) and the holes in the plurality of _third quantum boxes (QD ₃ ) are transferred to the plurality of second holes.
Of moving in the quantum box (QD _2), electrons from each of the second quantum boxes (QD ₂₎ - and to perform output by obtaining the observed light emission by hole recombination emission intensity distribution It is characterized by that. An information processing method according to a fourth aspect of the present invention provides a plurality of first information items in the first plane.
Quantum boxes that allow conduction of electrons between them are provided, and in the second plane corresponding to the plurality of first quantum boxes,
A plurality of second quantum boxes between which electrons and positive
A plurality of second holes are provided that do not allow the conduction of holes .
A plurality of third quantum boxes in the third plane corresponding to the quantum boxes of
A is what conduction of holes is allowed provided between them, by applying a bias voltage to the plurality of first quantum box side is a plurality of third potential higher than the quantum box side of the light irradiation
The second electrons in the quantum box selected by - generating a hole pairs, by increasing the bias voltage, corresponding to the second electrons and holes pairs generated in quantum box selected by the light irradiation, respectively To the first quantum box and the third quantum box, the electrons are conducted between the plurality of first quantum boxes, and the holes are conducted between the plurality of third quantum boxes. To remove electrons in the plurality of first quantum boxes and holes in the plurality of third quantum boxes into the plurality of second quantum boxes, Electronic-
The feature is that the light emission intensity distribution is obtained by observing light emission due to hole recombination. An information processing method according to a fifth aspect of the present invention has a plurality of first quantum boxes in a first plane and a plurality of second quantum boxes corresponding to a plurality of first quantum boxes in a second plane. And a semiconductor structure having a plurality of third quantum boxes corresponding to the plurality of second quantum boxes in the third plane, and at least the second quantum boxes selected by light irradiation are provided. A plurality of first quantum boxes that generate a pair of electrons and holes
So that the side has a higher potential than the sides of the multiple third quantum boxes
By applying a bias voltage , at least one electron is moved to the first quantum box, at least one hole is moved to the third quantum box, and at least one positive hole is moved between the quantum boxes in the third plane. The hole is moved, at least one electron is moved between the quantum boxes in the first plane, and the bias voltage is substantially
Of at least one electron and at least one hole are returned to the second quantum box, and at least one pair of electron and hole are combined to generate an information signal.

[0009]

According to the quantum box assembly element according to the first aspect of the present invention configured as described above, an electron and a hole generated as a pair in the _second quantum box (QD ₂ ) selected by light irradiation or the like. Corresponding to the first quantum box (QD ₁ ) and the third quantum box
Move the quantum box (QD _3), by conduction between these electrons and holes each of a plurality of first quantum box (QD ₁₎ and between the plurality of third quantum boxes (QD _3), Information processing can be performed according to the arrangement of the plurality of first quantum boxes (QD ₁ ) and the plurality of third quantum boxes (QD ₃ ). By allowing electrons and holes to participate in information processing in this way, it is possible to increase the degree of freedom in designing the quantum box assembly element.

According to the quantum box assembly element of the second aspect of the present invention constructed as described above, the first quantum element is formed by the type I heterojunction superlattice such as AlGaAs / GaAs heterojunction which can be easily formed by heteroepitaxial growth. Since the box (QD ₁ ), the second quantum box (QD ₂ ) and the third quantum box (QD ₃ ) are formed, the quantum box collective element can be easily manufactured.

According to the quantum box assembly element according to the third aspect of the present invention constructed as described above, the second quantum box (QD ₂ ) is irradiated with light to generate electron-hole pairs. Electrons injected from the first quantum box (QD ₁ ) corresponding to the _second quantum box (QD ₂ ) and the corresponding third quantum box
It is possible to realize a quantum box assembly element of optical input and optical output that outputs information by light emission due to recombination of holes injected from the quantum box (QD ₃ ). Configured as above
According to the information processing method according to the fourth and fifth inventions
For example, information processing can be performed using the quantum box assembly element described above.
It can be carried out.

[0012]

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings.

In this embodiment, generally, 1
A quantum box capable of accommodating only one electron among quantum boxes capable of accommodating more than one electron is specifically called a quantum dot, and an element in which a plurality of these quantum dots are combined is called a quantum dot aggregate element.

FIG. 1 shows a quantum dot assembly device according to an embodiment of the present invention.

As shown in FIG. 1, in the quantum dot assembly device according to this embodiment, a semi-insulating GaAs substrate 1 is used.
An n-type GaAs layer 2 used as an electrode for applying a bias voltage is formed on the Al, and Al as a barrier layer is formed thereon.
The As layer 3 is formed. On the AlAs layer 3, a plurality of box-shaped GaAs layers 4 as well layers are formed as xy.
An AlGaAs layer 5 as a barrier layer is formed in an array shape in a plane parallel to the plane in a predetermined array pattern and between the GaAs layers 4. These Ga
An AlAs layer 6 as a barrier layer is formed on the As layer 4 and the AlGaAs layer 5. A box-shaped GaAs layer 7 as a well layer is embedded in a portion of the AlAs layer 6 corresponding to the GaAs layer 4. Furthermore, A
A box-shaped GaAs layer 8 as a well layer is formed on the 1As layer 6 in an array corresponding to the GaAs layer 7, and AlGa as a barrier layer is formed between these GaAs layers 8.
The As layer 9 is embedded. And these GaA
An AlAs layer 10 as a barrier layer is formed on the s layer 8 and the AlGaAs layer 9.

In this case, the GaAs layer 4 and the GaAs layer 4 are parallel to the substrate surface, that is, in the x and y directions.
The widths of the layer 7 and the GaAs layer 8 are equal to each other, but GaA in the direction perpendicular to the substrate surface, that is, in the z direction.
The width of the s layer 7 is larger than the widths of the GaAs layer 4 and the GaAs layer 8. Here, the widths of the GaAs layer 4 and the GaAs layer 8 in the direction perpendicular to the substrate surface, that is, in the z direction are selected to be the same.

In this embodiment, the GaAs layer 8 as the well layer is the AlAs layer 6 and AlGa as the barrier layers.
The structure surrounded by the As layer 9 and the AlAs layer 10 forms the quantum dot QD ₁ in the upper stage of FIG. 1, that is, the first stage. As described later, this first-stage quantum dot QD
The array of ₁ is used for conduction of electrons for information processing. Further, the quantum dots QD ₂ in the middle stage in FIG. 1, that is, the second stage are formed by the structure in which the GaAs layer 7 as the well layer is surrounded by the AlAs layer 6 as the barrier layer. This second-stage quantum dot QD ₂ is the first-stage quantum dot QD ₁
Is formed at a position corresponding to. As will be described later, this second array of quantum dots QD ₂ is used for inputting information by irradiation of light. Furthermore, GaA as a well layer
The structure in which the s-layer 4 is surrounded by the AlAs layer 3, the AlGaAs layer 5, and the AlAs layer 6 as the barrier layer forms the quantum dot QD ₃ in the lower stage of FIG. 1, that is, the third stage. As will be described later, this array of quantum dots QD _{3 in} the third stage is used for conduction of holes for information processing.

In this case, the first-stage quantum dot QD ₁ , the second-stage quantum dot QD _2, and the third-stage quantum dot QD
_The AlGaAs / GaAs heterojunction and AlAs / GaAs heterojunction that compose ₃ are both type I heterojunction superlattices.

Although not shown, the AlAs layer 10
An electrode for applying a bias voltage is formed on the above. This electrode is formed of a metal or a transparent electrode material such as ITO (Indium-Tin Oxide). When the electrode is formed by metal, in order to enable incidence of light for input later in the quantum dot QD ₂ of the second stage, the quantum dot QD ₂ of the second stage of the electrode An opening is previously formed in the corresponding portion.

FIG. 2 shows an energy band diagram in the direction along the line α and the direction along the line γ in FIG. E _c and E _{v in} FIG. 2 represent the energy at the lower end of the conduction band and the energy at the upper end of the valence band (the same applies hereinafter). As can be seen from FIG. 2, in this case, the direction along the line α in FIG. 1, that is, the direction connecting the adjacent first-stage quantum dots QD ₁ and the direction along the line γ in FIG. 1, that is, the adjacent third stage. AlGaAs / Ga in the direction connecting the quantum dots QD ₃
The height of the potential barrier in the As heterojunction is quite small, and therefore the coupling strength between the quantum dots QD _{1 in the first} stage and between the quantum dots QD _{3 in the} third stage is strong. Then, conduction of electrons or holes by tunneling is allowed between the quantum dots QD _{1 in the first} stage and between the quantum dots QD _{3 in the} third stage. In FIG. 2, a quantum level corresponding to the ground state of the first quantum dot QD ₁ electronic indicated by a broken line in the conduction band, the quantum corresponding to the ground state of the first hole of the quantum dots QD ₁ The levels are indicated by broken lines in the valence band (the same applies below).

An energy band diagram in the direction along the line β in FIG. 1 is shown in FIG. As can be seen from FIG. 3, the quantum dots QD _{2 in the} direction along the line β in FIG.
The height of the potential barrier in the AlAs / GaAs heterojunction in the direction connecting them is considerably larger than the height of the potential barrier in the AlGaAs / GaAs heterojunction, and therefore the quantum dots QD _{2 in the} second stage
The strength of the bond between them is very weak. Therefore, conduction of electrons or holes due to tunneling is not substantially allowed between the second-stage quantum dots QD ₂ .

An energy band diagram in the direction along the line δ in FIG. 1 is shown in FIG. As can be seen from FIG. 4, in this case, the ground state energy of the electrons of the second-stage quantum dot QD ₂ is the energy of the ground states of the electrons of the first-stage quantum dot QD ₁ and the third-stage quantum dot QD _3. Is lower than. Similarly, the ground state energy of holes in the second-stage quantum dot QD ₂ is lower than the ground state energy of holes in the first-stage quantum dot QD ₁ and the third-stage quantum dot QD _3. There is. As described above, this is the quantum dot QD of the second stage with respect to the direction along the line δ.
_This is because the dimension of ₂ is larger than the dimensions of the quantum dots QD _{1 in the} first stage and the quantum dots QD _{3 in} the third stage.

Next, the operation principle of the quantum dot assembling device according to this embodiment constructed as described above will be explained.

First, at the time of input, the n-type GaAs layer 2 and A
A bias voltage is applied between the electrode (not shown) on the 1As layer 10 so that the potential of this electrode is slightly higher than the potential of the n-type GaAs layer 2. At this time, the energy band in the direction along the line δ in FIG. 1 is slightly inclined as shown in FIG. Next, in this state, as shown in FIG. 6, the second-stage quantum dot QD selected according to the information to be input.
To _2, the two-stage electron quantum dot QD ₂ - irradiated with monochromatic light of a wavelength that resonates with hole pair generating energy, electrons in the quantum dot QD ₂ (e ^{-) -} hole (h ⁺ ) Generate a pair. As is apparent from FIG. 6, this photon energy of monochromatic light does not generate electron-hole pairs in the quantum dots QD _{1 in the} first stage and the quantum dots QD ₃ in the third stage. Therefore, the quantum dots QD
Only in ₂ are electron-hole pairs generated. The monochromatic light irradiation can be specifically performed by using, for example, laser light having a sufficiently small spot diameter.

In this case, this light irradiation causes the quantum dots Q
Both D electrons and holes pairs generated in _2, the high potential barrier due to AlAs layers 6 is a barrier layer of the quantum dot QD _2, it can not be moved out of the quantum dot QD _2. Further, since the electrons and holes in the quantum dots QD ₂ are spatially separated by the electric field in the z direction due to the above-mentioned bias voltage, the recombination rate of the electrons and holes pair-generated by the light irradiation is low. .

As described above, the electron-hole pairs are generated in the selected second-stage quantum dots QD ₂ by scanning with monochromatic light such as laser light, and the initial electron distribution and the initial electron distribution are obtained. Input the hole distribution. The initial electron distribution and the initial hole distribution are the same. Here, these initial electron distribution and initial hole distribution are f
It is expressed as (x, y).

As described above, the second-stage quantum dot QD
Initial electron distribution and initial hole distribution f to array ₂
After the input of (x, y) is completed, the n-type GaAs layer 2 and A
The above-mentioned bias voltage applied between the 1As layer 10 and the electrode is increased. As a result, the energy band in the direction along the line δ in FIG. 1 is greatly inclined as shown in FIG. Here, due to the electric field in the z direction due to the bias voltage,
While the quantum level corresponding to the ground state of the electron in the conduction band of the first-stage quantum dot QD ₁ becomes lower than the quantum level corresponding to the ground state of the electron in the conduction band of the second-stage quantum dot QD ₂ , The quantum level corresponding to the ground state of holes in the valence band of the third-stage quantum dot QD ₃ is the second-stage quantum dot QD.
_It is assumed that the quantum level becomes lower than the quantum level corresponding to the ground state of holes in the valence band of ₂ . Then, the second-stage quantum dot QD
The electrons in ₂ simultaneously transit to the corresponding quantum dot QD ₁ in the _first stage, and the holes in the _second quantum dot QD ₂ simultaneously transit to the corresponding quantum dot QD ₃ in the third stage.

As described above, the first-stage quantum dot QD
_The electrons moved to ₁ are conducted by tunneling between the quantum dots QD ₁ due to the small height of the potential barrier between the quantum dots QD ₁ as described above. The conduction of this electron is due to this quantum dot QD
_It happens according to the arrangement of ₁ . Similarly, holes move to the quantum dot QD ₃ of the third stage, by the height of the potential barrier between these quantum dots QD ₃ is small as previously mentioned, tunneling between these quantum dots QD ₃ Conducted by. The conduction of the holes occurs according to the arrangement of the quantum dots QD ₃ .

In this case, the electrons and holes have at least different effective masses from each other, and the quantum dot QD
Quantum dots Q for tunnel barrier height and holes between ₁
Since the height of the tunnel barrier between D ₃ is different from each other, the distribution of electrons in the array of quantum dots QD _{1 in} the first stage and the distribution of holes in the array of quantum dots QD _{3 in} the third stage have different time changes. To do. Therefore, the initial electron distribution f (x, y) changes to f (x, y) → g (x, y), and the initial hole distribution f (x, y) f (x, y) → h ( x (y), g (x, y) ≠ h (x, y). The above is information processing by conduction of electrons in the array of quantum dots QD _{1 in} the first stage and conduction of holes in the array of quantum dots QD _{3 in} the third stage.

Next, at the time of output, the n-type GaAs layer 2 and A
The bias voltage between the electrodes on the 1As layer 10 is set to zero. At this time, the energy band in the direction along the line δ in FIG. 1 is as shown in FIG. As a result, as shown in FIG. 8, the quantum state corresponding to the ground state of the electron in the conduction band of the first-stage quantum dot QD ₁ corresponds to the ground state of the electron in the conduction band of the second-stage quantum dot QD _2. The quantum level corresponding to the ground state of holes in the valence band of the third-stage quantum dot QD ₃ is higher than that of the quantum dot QD ₂ of the second-stage quantum dot QD _2. It is again higher than the quantum level corresponding to the ground state of the hole. As a result, the electrons in the first-stage quantum dot QD ₁
The quantum dots Q of the third stage while simultaneously transiting to D _2.
The holes in D ₃ simultaneously transit to the corresponding second-stage quantum dots QD ₂ . As a result, electron-hole recombination occurs in the quantum dot QD ₂ in which electrons and holes coexist, and light emission (hν) occurs as shown in FIG. The emission intensity distribution in this case is the distribution of electrons g (x, y) in the array of quantum dots QD _{1 in} the _first row and the distribution of holes h (x, y in the array of quantum dots QD _{3 in} the third row immediately before output. y) and the product. That is, the emission intensity distribution is g (x, y) h (x, y). This can be output information.

As described above, the input distribution f (x, y)
The output distribution g (x, y) h (x, y) can be obtained from

As described above, according to this embodiment, light is applied to the array of the second-stage quantum dots QD ₂ to input light, and the electron conduction and the third electron in the first-stage quantum dot QD ₁ array are performed. It is possible to realize a quantum dot assembly device that performs information processing by conduction of holes in the array of quantum dots QD ₃ and outputs by emitting light from the array of quantum dots QD _{2 in} the second stage. This quantum dot assembly element has a high degree of freedom in design because electrons and holes are involved in information processing.

Next, a method of manufacturing the quantum dot assembly element according to this embodiment configured as described above will be described.

First, as shown in FIG. 9, semi-insulating GaA
On the substrate 1, for example, metal organic chemical vapor deposition (MOCV)
D) method, n-type GaAs layer 2, AlAs layer 3, Ga
The As layer 4, the AlAs layer 6a, the GaAs layer 7, the AlAs layer 6b, the GaAs layer 8 and the AlAs layer 10a are sequentially epitaxially grown. The n-type GaAs layer 2 has a thickness of, for example, about 1000 nm, and the AlAs layer 3 has a thickness of, for example, about 100 nm.

Next, as shown in FIG. 10, the AlAs layer 1
A resist pattern 11 having a shape corresponding to the _first- stage quantum dot QD ₁ , the second-stage quantum dot QD _2, and the third-stage quantum dot QD ₃ is formed on 0a. The resist pattern 11 is formed, for example, by selectively irradiating the AlAs layer 10a with an electron beam having a sufficiently small spot diameter in a predetermined source gas atmosphere in a vacuum-exhausted sample chamber of an electron beam irradiation apparatus. Then, the decomposition product of the raw material gas is deposited on the irradiation part.

Next, using the resist pattern 11 thus formed as a mask, the AlAs layer 10a, the GaAs layer 8 and the AlAs layer 10a are formed by anisotropic dry etching such as reactive ion etching (RIE).
Layer 6b, GaAs layer 7, AlAs layer 6a and GaAs
Layer 4 is etched sequentially in the direction perpendicular to the substrate surface. This etching is overetched so that the GaAs layers 4 are completely separated from each other. Thus, as shown in FIG. 11, the GaAs layer 4 and the AlAs layer 6 are formed.
a, the GaAs layer 7, the AlAs layer 6b, the GaAs layer 8 and the AlAs layer 10a are patterned into a rectangular column shape.

Next, as shown in FIG. 12, for example, MOC
By the VD method, the AlGaAs layer 5, the AlAs layer 6c, and the AlG layer 5c are grown under the condition that the growth does not occur on the side wall perpendicular to the substrate surface.
The aAs layer 9 and the AlAs layer 10b are sequentially epitaxially grown to form a square columnar GaAs layer 4 and an AlAs layer 6.
a, the GaAs layer 7, the AlAs layer 6b, the GaAs layer 8 and the AlAs layer 10a are filled.

Thereafter, electrodes (not shown) are formed on the AlAs layers 10a and 10b.

As described above, the quantum dot assembly element shown in FIG. 1 is completed.

Although one embodiment of the present invention has been specifically described above, the present invention is not limited to the above embodiment, and various modifications can be made based on the technical idea of the present invention. .

For example, it goes without saying that the method of manufacturing the quantum dot assembly element described in the above-mentioned one embodiment is merely an example, and other manufacturing methods may be used.

Further, in the above-mentioned embodiment, AlGaAs, AlAs and GaAs are used as the material of the quantum dot assembly element, but as the material of this quantum dot assembly element, more generally, the quantum box assembly element. Semiconductor materials other than these may be used.

[0043]

As described above, according to the present invention,
Information is input by light irradiation, and the desired information processing is performed by conducting the electrons and holes generated by the light irradiation in pairs in the quantum box arrays provided in different planes by tunneling. Thus, it is possible to realize a quantum box assembly element that can output information and has a high degree of freedom in design. Also this
Providing an information processing method using such a quantum box assembly element
be able to.

[Brief description of drawings]

FIG. 1 is a perspective view showing a quantum dot assembly element according to an embodiment of the present invention.

FIG. 2 is an energy band diagram in a direction along a line α in FIG. 1 and a direction along a line γ in FIG.

FIG. 3 is an energy band diagram in a direction along a line β in FIG.

FIG. 4 is an energy band diagram in a direction along a line δ in FIG.

5 is an energy band diagram for explaining an input method of the quantum dot assembly device shown in FIG. 1. FIG.

6 is an energy band diagram for explaining an input method of the quantum dot assembly device shown in FIG.

7 is an energy band diagram for explaining the operation of the quantum dot assembly element shown in FIG. 1 after input and before information processing.

8 is an energy band diagram for explaining an output method of the quantum dot assembly device shown in FIG.

9 is a perspective view for explaining a method of manufacturing the quantum dot aggregate device shown in FIG. 1. FIG.

10 is a perspective view for explaining a method of manufacturing the quantum dot aggregate device shown in FIG. 1. FIG.

FIG. 11 is a perspective view for explaining a method of manufacturing the quantum dot aggregate device shown in FIG. 1.

FIG. 12 is a perspective view for explaining the method of manufacturing the quantum dot aggregate device shown in FIG. 1.

[Explanation of symbols]

1 Semi-insulating GaAs substrate 2 n-type GaAs layer 3, 6, 10 AlAs layer 4, 7, 8 GaAs layer 5, 9 AlGaAs layer

Claims (5)

(57) [Claims] 1. A plurality of first quantities provided in a first plane.
Child box that allows conduction of electrons between them
And a plurality of second quantum boxes provided corresponding to the plurality of first quantum boxes in the second plane, and electrons and
And a plurality of third quantum boxes provided correspondingly to the plurality of second quantum boxes in the third plane, and positive holes between them. Transmission of holes
And the plurality of first quantum box sides are the third quantum box sides.
The bias voltage is applied so that the potential becomes higher than
In the state, electrons are emitted to the second quantum box selected by light irradiation.
-Initial electron distribution and initial by generating hole pairs
The hole distribution is input, the bias voltage is increased, and the light irradiation causes the selection.
Pair-generated electrons in the selected second quantum box and
The first quantum box and the first quantum box which respectively correspond to holes.
By moving to the quantum box of 3
And the initial hole distribution to the plurality of first quanta, respectively.
Transfer to the box and the third quantum boxes above, and then
Note that when the above electrons are conducted between a plurality of first quantum boxes,
To conduct the holes between the plurality of third quantum boxes.
Information processing is carried out by removing the bias voltage by removing the bias voltage.
In the first quantum box of the number and the plurality of third quanta
Move the holes in the box into the second quantum boxes
By electron-hole recombination from each of the above second quantum boxes
Output by observing the emitted light and obtaining the emission intensity distribution
A quantum box assembly device characterized by being performed . 2. The quantum box according to claim 1, wherein the first quantum box, the second quantum box and the third quantum box are formed by a type I heterojunction superlattice. Collective element. 3. The electron-hole of the second quantum box is applied with a bias voltage applied so that the side of the plurality of first quantum boxes has a higher potential than the side of the plurality of third quantum boxes. An initial electron distribution and an initial hole distribution are input by irradiating the selected second quantum box with light having a wavelength that resonates with the pair production energy to generate an electron-hole pair, and the bias voltage is set to By moving electrons and holes pair-generated in the second quantum box selected by the incidence of the light to the corresponding first quantum box and the third quantum box, respectively. The initial electron distribution and the initial hole distribution are transferred to the plurality of first quantum boxes and the plurality of third quantum boxes, respectively, and thereafter,
Together to conduct the electrons between said plurality of first quantum box performs information processing by conducting the hole between the plurality of third quantum box, substantially removing the bias voltage To move the electrons in the plurality of first quantum boxes and the holes in the plurality of third quantum boxes into the plurality of second quantum boxes, so that the electrons from the respective second quantum boxes are moved. The quantum box assembly element according to claim 1 or 2, wherein the quantum box assembly element is configured to perform output by observing light emission due to hole recombination and obtaining an emission intensity distribution. 4. A plurality of first quantum boxes are included in the first plane .
I provided that electron conduction is allowed between them, the second plane in correspondence with the plurality of first quantum box, a plurality
The second quantum box of, between which electrons and holes
What conduction is not substantially allowed provided the third plane in correspondence with the plurality of second quantum boxes, multiple
Is the third quantum box of and allows conduction of holes between them
A bias voltage is applied so that the side of the plurality of first quantum boxes has a higher potential than the side of the plurality of third quantum boxes, and the second quantum box selected by light irradiation is applied. An electron-hole pair is generated, the bias voltage is increased, and the electron and hole pair-generated in the second quantum box selected by the light irradiation respectively correspond to the first quantum. Box and the third quantum box, the electrons are conducted between the plurality of first quantum boxes and the holes are conducted between the plurality of third quantum boxes, and the bias voltage is substantially The first of the plurality of
Of the electrons in the quantum boxes and holes in the plurality of third quantum boxes into the plurality of second quantum boxes, and by electron-hole recombination from each of the second quantum boxes. An information processing method characterized by observing luminescence and obtaining a luminescence intensity distribution. 5. A plurality of first quantum boxes in a first plane, and a plurality of second quantum boxes corresponding to the plurality of first quantum boxes in a second plane, The plurality of second portions in the third plane
A semiconductor structure having a plurality of third quantum boxes corresponding to the plurality of quantum boxes, and at least a pair of electrons and holes are generated in the second quantum box selected by light irradiation , The side of the quantum box is the side of the plurality of third quantum boxes
The bias voltage should be applied so that the potential becomes higher than
And move at least one electron to the first quantum box, move at least one hole to the third quantum box, and move at least one hole between the quantum boxes in the third plane. At least one electron is moved between the quantum boxes in the first plane and the bias voltage is substantially removed to move at least one electron and at least one hole into the second quantum box. And an information signal is generated by combining at least a pair of electrons and holes to generate an information signal.